System and method for making concentration measurements within a sample material using orbital angular momentum

ABSTRACT

An apparatus for identifying a concentration of a specific material within a first material includes an input for receiving a signal after the signal passes through the first material. The signal has at least one orthogonal function therein and the at least one orthogonal function comprises at least one of an orbital angular momentum function or a Laguerre-Gaussian function. A detector detects the at least one orthogonal function within the signal, determines the concentration of the specific material within the first material based upon the detected at least one orthogonal function and generates an indication responsive to the determination. An output provides for an output of the generated indication.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a Continuation of U.S. patent application Ser. No. 15/049,594, filed on Feb. 22, 2016, entitled SYSTEM AND METHOD FOR MAKING CONCENTRATION MEASUREMENTS WITHIN A SAMPLE MATERIAL USING ORBITAL ANGULAR MOMENTUM (Atty. Dkt. No. NXGN-32803), which is a Continuation of U.S. patent application Ser. No. 14/339,836, filed on Jul. 24, 2014, entitled SYSTEM AND METHOD FOR MAKING CONCENTRATION MEASUREMENTS WITHIN A SAMPLE MATERIAL USING ORBITAL ANGULAR MOMENTUM, now U.S. Pat. No. 9,267,877, issued on Feb. 23, 2016 (Atty. Dkt. No. NXGN-32196), which claims benefit of U.S. Provisional Application No. 61/951,834, filed Mar. 12, 2014, entitled CONCENTRATION MEASUREMENTS USING PHOTON ORBITAL ANGULAR MOMENTUM (Atty. Dkt. No. NXGN-32089), the specifications of which are incorporated by reference herein in their entirety.

TECHNICAL FIELD

The present invention relates to concentration measurements of various organic and non-organic materials, and more particularly, to concentration measurements of organic and non-organic materials using the orbital angular momentum of waves passed through a sample of the material.

BACKGROUND

Concentration measurements of organic and non-organic materials within human tissue are an increasingly important aspect of healthcare for individuals. The development of non-invasive measurement techniques for monitoring biological and metabolic agents within human tissue is an important aspect of diagnosis therapy of various human diseases and may play a key role in the proper management of diseases.

One example of a biological agent that may be monitored for within human tissue is glucose. Glucose (C₆H₁₂O₆) is a monosaccharide sugar and is one of the most important carbohydrate nutrient sources. Glucose is fundamental to almost all biological processes and is required for the production of ATP adenosine triphosphate and other essential cellular components. The normal range of glucose concentration within human blood is 70-160 mg/dl depending on the time of the last meal, the extent of physical tolerance and other factors. Freely circulating glucose molecules stimulate the release of insulin from the pancreas. Insulin helps glucose molecules to penetrate the cell wall by binding two specific receptors within cell membranes which are normally impermeable to glucose.

One disease associated with issues related to glucose concentrations is diabetes. Diabetes is a disorder caused by the decreased production of insulin, or by a decreased ability to utilize insulin and transport the glucose across cell membranes. As a result, a high potentially dangerous concentration of glucose can accumulate within the blood (hyperglycemia) during the disease. Therefore, it is of great importance to maintain blood glucose concentration within a normal range in order to prevent possible severe physiological complications.

One significant role of physiological glucose monitoring is the diagnosis and management of several metabolic diseases, such as diabetes mellitus (or simply diabetes). There are a number of invasive and non-invasive techniques presently used for glucose monitoring. The problem with existing non-invasive glucose monitoring techniques is that a clinically acceptable process has not yet been determined. Standard techniques from the analysis of blood currently involve an individual puncturing a finger and subsequent analysis of collected blood samples from the finger. In recent decades, non-invasive blood glucose monitoring has become an increasingly important topic of investigation in the realm of biomedical engineering. In particular, the introduction of optical approaches has caused some advances within the field. Advances in optics have led to a focused interest in optical imaging technologies and the development of non-invasive imaging systems. The application of optical methods to monitoring in cancer diagnostics and treatment is also a growing field due to the simplicity and low risk of optical detection methods.

Many optical techniques for sensing different tissue metabolites and glucose in living tissue have been in development over the last 50 years. These methods have been based upon florescent, near infrared and mid-infrared spectroscopy, Raman spectroscopy, photoacoustics, optical coherence tomography and other techniques. However, none of these techniques that have been tried have proved completely satisfactory.

Another organic component lending itself to optical material concentration sensing involves is human skin. The defense mechanisms of human skin are based on the action of antioxidant substances such as carotenoids, vitamins and enzymes. Beta carotene and lycopene represent more than 70% of the carotenoids in the human organism. The topical or systematic application of beta carotene and lycopene is a general strategy for improving the defense system of the human body. The evaluation and optimization of this treatment requires the measurement of the b-carotene and lycopene concentrations in human tissue, especially in the human skin as the barrier to the environment.

Thus, an improved non-invasive technique enabling the detection of concentrations of various materials within a human body or other types of samples would have a number of applications within the medical field.

SUMMARY

The present invention, as disclosed and described herein, in one aspect thereof comprises an apparatus for identifying a concentration of a specific material within a first material. An input receives a signal after the signal passes through the first material. The signal has at least one orthogonal function therein and the at least one orthogonal function comprises at least one of an orbital angular momentum function or a Laguerre-Gaussian function. A detector detects the at least one orthogonal function within the signal, determines the concentration of the specific material within the first material based upon the detected at least one orthogonal function and generates an indication responsive to the determination. An output provides for an output of the generated indication.

BRIEF DESCRIPTION OF THE DRAWINGS

For a more complete understanding, reference is now made to the following description taken in conjunction with the accompanying Drawings in which:

FIG. 1 illustrates a general representation of a manner for determining a concentration of a particular material within a sample using a light beam or other wave;

FIG. 2 illustrates a light beam having orbital angular momentum imparted thereto;

FIG. 3 illustrates a series of parallel wavefronts;

FIG. 4 illustrates a wavefront having a Poynting vector spiraling around a direction of propagation of the wavefront;

FIG. 5 illustrates a plane wavefront while FIG. 6 helical wavefront;

FIG. 7 illustrates a plane wave having only variations in the spin vector;

FIG. 8 illustrates the application of a unique orbital angular momentum to a wave;

FIGS. 9a-9c illustrate the differences between signals having different orbital angular momentum applied thereto;

FIG. 10 illustrates the propagation of Poynting vectors for various eigenmodes;

FIG. 11 illustrates a block diagram of an apparatus for providing concentration measurements of various materials using orbital angular momentum;

FIG. 12 illustrates an emitter of the system of FIG. 11;

FIG. 13 illustrates a fixed orbital angular momentum generator of the system of FIG. 11;

FIGS. 14a-14d illustrate various holograms for use in applying an orbital angular momentum to a plane wave signal;

FIG. 15 illustrates the relationship between Hermite-Gaussian modes and Laguerre-Gaussian modes;

FIG. 16 illustrates super-imposed holograms for applying orbital angular momentum to a signal;

FIG. 17 illustrates a tunable orbital angular momentum generator for use in the system of FIG. 11;

FIG. 18 illustrates a block diagram of a tunable orbital angular momentum generator including multiple hologram images therein;

FIG. 19 illustrates the manner in which the output of the OAM generator may be varied by applying different orbital angular momentums thereto;

FIG. 20 illustrates an alternative manner in which the OAM generator may convert a Hermite-Gaussian beam to a Laguerre-Gaussian beam;

FIG. 21 illustrates the manner in which holograms within an OAM generator may twist a beam of light;

FIG. 22 illustrates the manner in which a sample receives an OAM twisted wave and provides an output wave having a particular OAM signature;

FIG. 23 illustrates the manner in which orbital angular momentum interacts with a molecule around its beam axis;

FIG. 24 illustrates a block diagram of the matching circuitry for amplifying a received orbital angular momentum signal;

FIG. 25 illustrates the manner in which the matching module may use non-linear crystals in order to generate a higher order orbital angular momentum light beam;

FIG. 26 illustrates a block diagram of an orbital angular momentum detector and user interface;

FIG. 27 illustrates the effect of sample concentrations upon the spin angular polarization and orbital angular polarization of a light beam passing through a sample;

FIG. 28 more particularly illustrates the process that alters the orbital angular momentum polarization of a light beam passing through a sample;

FIG. 29 provides a block diagram of a user interface of the system of FIG. 11;

FIG. 30 illustrates a network configuration for passing around data collected via devices such as that illustrated in FIG. 11; and

FIG. 31 provides a block diagram of a more particular embodiment of an apparatus for measuring the concentration of glucose using orbital angular momentum.

DETAILED DESCRIPTION

Referring now to the drawings, wherein like reference numbers are used herein to designate like elements throughout, the various views and embodiments of system and method for making concentration measurements within a sample material using orbital angular momentum are illustrated and described, and other possible embodiments are described. The figures are not necessarily drawn to scale, and in some instances the drawings have been exaggerated and/or simplified in places for illustrative purposes only. One of ordinary skill in the art will appreciate the many possible applications and variations based on the following examples of possible embodiments.

Referring now to the drawings, and more particularly to FIG. 1, there is illustrated a general representation of the manner in which the concentration of a particular material sample 102 may be monitored using orbital angular momentum applied to a light beam or other wave transmitted through the material sample 102. The material sample 102 has a beam 104 shined through the length of the material sample 102. After passing through the material sample 102, the exiting beam 106 leaves the material sample and may be analyzed to determine various concentration characteristics within the material sample 102. The manner in which the different characteristics of the material sample 102 may be determined within the exiting beam 106 is achieved with respect to an analysis of the orbital angular momentum signatures that are imparted to the exiting beam 106 by the concentrations within the material sample 102.

Referring now also to FIG. 2, there is illustrated one embodiment of a beam for use with the system. A light beam 104 consists of a stream of photons 202 within the light beam 104. Each photon has an energy ±

and a linear momentum of ±

k which is directed along the light beam axis 204 perpendicular to the wavefront. Independent of the frequency, each photon 202 within the light beam has a spin angular momentum 206 of ±

aligned parallel or antiparallel to the direction of light beam propagation. Alignment of all of the photons 202 spins gives rise to a circularly polarized light beam. In addition to the circular polarization, the light beams also may carry an orbital angular momentum 208 which does not depend on the circular polarization and thus is not related to photon spin.

Lasers are widely used in optical experiments as the source of well-behaved light beams of a defined frequency. A laser may be used for providing the light beam 104 as described with respect to FIG. 1. The energy flux in any light beam 104 is given by the Poynting vector which may be calculated from the vector product of the electric and magnetic fields within the light beam. In a vacuum or any isotropic material, the Poynting vector is parallel to the wave vector and perpendicular to the wavefront of the light beam. In a normal laser light, the wavefronts 300 are parallel as illustrated in FIG. 3. The wave vector and linear momentum of the photons are directed along the axis in a z direction 302. The field distributions of such light beams are paraxial solutions to Maxwell's wave equation but although these simple beams are the most common, other possibilities exist.

For example, beams that have l intertwined helical fronts are also solutions of the wave equation. The structure of these complicated beams is difficult to visualize, but their form is familiar from the l=3 fusilli pasta. Most importantly, the wavefront has a Poynting vector and a wave vector that spirals around the light beam axis direction of propagation as illustrated in FIG. 4 at 402.

A Poynting vector has an azimuthal component on the wave front and a non-zero resultant when integrated over the beam cross-section. The spin angular momentum of circularly polarized light may be interpreted in a similar way. A beam with a circularly polarized planer wave front, even though it has no orbital angular momentum, has an azimuthal component of the Poynting vector proportional to the radial intensity gradient. This integrates over the cross-section of the light beam to a finite value. When the beam is linearly polarized, there is no azimuthal component to the Poynting vector and thus no spin angular momentum.

Thus, the momentum of each photon 202 within the light beam 104 has an azimuthal component. A detailed calculation of the momentum involves all of the electric fields and magnetic fields within the light beam, particularly those electric and magnetic fields in the direction of propagation of the beam. For points within the beam, the ratio between the azimuthal components and the z components of the momentum is found to be l/kr. The linear momentum of each photon 202 within the light beam 104 is given by

k, so if we take the cross product of the azimuthal component within a radius vector, r, we obtain an orbital momentum for a photon 202 of l

. Note also that the azimuthal component of the wave vectors is l/r and independent of the wavelength.

Referring now to FIGS. 5 and 6, there are illustrated plane wavefronts and helical wavefronts. Ordinarily, laser beams with plane wavefronts 502 are characterized in terms of Hermite-Gaussian modes. These modes have a rectangular symmetry and are described by two mode indices m 504 and n 506. There are m nodes in the x direction and n nodes in the y direction. Together, the combined modes in the x and y direction are labeled HG_(mn) 508. In contrast, as shown in FIG. 6 beams with helical wavefronts 602 are best characterized in terms of Laguerre-Gaussian modes which are described by indices I 603, the number of intertwined helices 604, and p, the number of radial nodes 606. The Laguerre-Gaussian modes are labeled LG_(mn) 610. For l≈0, the phase singularity on a light beam 104 results in 0 on axis intensity. When a light beam 104 with a helical wavefront is also circularly polarized, the angular momentum has orbital and spin components, and the total angular momentum of the light beam is (l±

) per photon.

Using the orbital angular momentum state of the transmitted energy signals, physical information can be embedded within the electromagnetic radiation transmitted by the signals. The Maxwell-Heaviside equations can be represented as:

${\nabla{\cdot E}} = \frac{\rho}{ɛ_{0}}$ ${\nabla{\times E}} = \frac{\partial B}{\partial t}$ ∇⋅B = 0 ${\nabla{\times B}} = {{ɛ_{0}\mu_{0}\frac{\partial E}{\partial t}} + {\mu_{0}{j\left( {t,x} \right)}\; {the}}}$

where ∇ is the del operator, E is the electric field intensity and B is the magnetic flux density. Using these equations, we can derive 23 symmetries/conserve quantities from Maxwell's original equations. However, there are only ten well-known conserve quantities and only a few of these are commercially used. Historically if Maxwell's equations where kept in their original quaternion forms, it would have been easier to see the symmetries/conserved quantities, but when they were modified to their present vectorial form by Heaviside, it became more difficult to see such inherent symmetries in Maxwell's equations.

The conserved quantities and the electromagnetic field can be represented according to the conservation of system energy and the conservation of system linear momentum. Time symmetry, i.e. the conservation of system energy can be represented using Poynting's theorem according to the equations:

$H = {{\sum\limits_{i}{m_{i}\gamma_{i}c^{2}}} + {\frac{ɛ_{0}}{2}{\int{d^{3}x\mspace{11mu} \left( {{E}^{2} + {c^{2}{B}^{2}}} \right)}}}}$ ${\frac{{dU}^{mech}}{dt} + \frac{{dU}^{em}}{dt} + {\oint_{s^{\prime}}{d^{2}x^{\prime}{\hat{n^{\prime}} \cdot S}}}} = 0$

The space symmetry, i.e., the conservation of system linear momentum representing the electromagnetic Doppler shift can be represented by the equations:

$P = {{\sum\limits_{i}{m_{i}\gamma_{i}v_{i}}} + {ɛ_{0}{\int{d^{3}x\mspace{11mu} \left( {E \times B} \right)}}}}$ ${\frac{{dp}^{mech}}{dt} + \frac{{dp}^{em}}{dt} + {\oint_{s^{\prime}}{d^{2}x^{\prime}{\hat{n^{\prime}} \cdot T}}}} = 0$

The conservation of system center of energy is represented by the equation:

$R = {{\frac{1}{H}{\sum\limits_{i}{\left( {x_{i} - x_{0}} \right)m_{i}\gamma_{i}c^{2}}}} + {\frac{ɛ_{0}}{2H}{\int{d^{3}x\mspace{11mu} \left( {x - x_{0}} \right)\left( {{E^{2}} + {c^{2}{B^{2}}}} \right)}}}}$

Similarly, the conservation of system angular momentum, which gives rise to the azimuthal Doppler shift is represented by the equation:

${\frac{{dJ}^{mech}}{dt} + \frac{{dJ}^{em}}{dt} + {\oint_{s^{\prime}}{d^{2}x^{\prime}{\hat{n^{\prime}} \cdot M}}}} = 0$

For radiation beams in free space, the EM field angular momentum J^(em) can be separated into two parts:

J ^(em)=ε₀∫_(V′) d ³ x′(E×A)+ε₀∫_(V′) d ³ x′E _(i)[(x′−x ₀)×∇]A _(i)

For each singular Fourier mode in real valued representation:

$J^{em} = {{{- i}\frac{ɛ_{0}}{2\omega}{\int_{V^{\prime}}{d^{3}{x^{\prime}\left( {E^{\star} \times E} \right)}}}} - {i\frac{ɛ_{0}}{2\omega}{\int_{V^{\prime}}{d^{3}x^{\prime}{E_{i}\left\lbrack {\left( {x^{\prime} - x_{0}} \right) \times \nabla} \right\rbrack}E_{i}}}}}$

The first part is the EM spin angular momentum S^(em), its classical manifestation is wave polarization. And the second part is the EM orbital angular momentum L^(em) its classical manifestation is wave helicity. In general, both EM linear momentum P^(em), and EM angular momentum J^(em)=L^(em)+S^(em) are radiated all the way to the far field.

By using Poynting theorem, the optical vorticity of the signals may be determined according to the optical velocity equation:

${{\frac{\partial U}{\partial t} + {\nabla{\cdot S}}} = 0},$

where S is the Poynting vector

S=1/4(E×H*+E*×H);

and U is the energy density

U=1/4(ε|E| ²+μ₀ |H| ²);

with E and H comprising the electric field and the magnetic field, respectively, and ε and μ₀ being the permittivity and the permeability of the medium, respectively. The optical vorticity V may then be determined by the curl of the optical velocity according to the equation:

$V = {{\nabla{\times v_{opt}}} = {\nabla{\times \left( \frac{{E \times H^{\star}} + {E^{\star} \times H}}{{ɛ{E}^{2}} + {\mu_{0}{H}^{2}}} \right)}}}$

Referring now to FIGS. 7 and 8, there are illustrated the manner in which a signal and an associated Poynting vector of the signal vary in a plane wave situation (FIG. 7) where only the spin vector is altered, and in a situation wherein the spin and orbital vectors are altered in a manner to cause the Poynting vector to spiral about the direction of propagation (FIG. 8).

In the plane wave situation, illustrated in FIG. 7, when only the spin vector of the plane wave is altered, the transmitted signal may take on one of three configurations. When the spin vectors are in the same direction, a linear signal is provided as illustrated generally at 704. It should be noted that while 704 illustrates the spin vectors being altered only in the x direction to provide a linear signal, the spin vectors can also be altered in the y direction to provide a linear signal that appears similar to that illustrated at 704 but in a perpendicular orientation to the signal illustrated at 704. In linear polarization such as that illustrated at 704, the vectors for the signal are in the same direction and have a same magnitude.

Within a circular polarization as illustrated at 706, the signal vectors 712 are 90 degrees to each other but have the same magnitude. This causes the signal to propagate as illustrated at 706 and provide the circular polarization 714 illustrated in FIG. 7. Within an elliptical polarization 708, the signal vectors 716 are also 90 degrees to each other but have differing magnitudes. This provides the elliptical polarizations 718 illustrated for the signal propagation 408. For the plane waves illustrated in FIG. 7A, the Poynting vector is maintained in a constant direction for the various signal configurations illustrated therein.

The situation in FIG. 8 illustrates when a unique orbital angular momentum is applied to a signal. When this occurs, Poynting vector S 810 will spiral around the general direction of propagation 812 of the signal. The Poynting vector 810 has three axial components S_(φ), S_(p) and S_(z) which vary causing the vector to spiral about the direction of propagation 612 of the signal. The changing values of the various vectors comprising the Poynting vector 810 may cause the spiral of the Poynting vector to be varied in order to enable signals to be transmitted on a same wavelength or frequency as will be more fully described herein. Additionally, the values of the orbital angular momentum indicated by the Poynting vector 410 may be measured to determine concentrations associated with particular materials being processed by a concentration scanning mechanism.

FIGS. 9a-9c illustrate the differences in signals having a different helicity (i.e., orbital angular momentum applied thereto). The differing helicities would be indicative of differing concentration of materials within a sample that a beam was being passed through. By determining the particular orbital angular momentum signature associated with a signal, the concentration amounts of the material could be determined. Each of the spiraling Poynting vectors associated with a signal 902, 904 and 906 provides a different-shaped signal. Signal 902 has an orbital angular momentum of +1, signal 904 has an orbital angular momentum of +3 and signal 906 has an orbital angular momentum of −4. Each signal has a distinct orbital angular momentum and associated Poynting vector enabling the signal to be indicative of a particular concentration of material that is associated with the detected orbital angular momentum. This allows determinations of concentrations of various types of materials to be determined from a signal since the orbital angular momentums are separately detectable and provide a unique indication of the concentration of the particular material that has affected the orbital angular momentum of the signal transmitted through the sample material.

FIG. 10 illustrates the propagation of Poynting vectors for various Eigen modes. Each of the rings 1020 represents a different Eigen mode or twist representing a different orbital angular momentum. Each of the different orbital angular momentums is associated with a particular concentration of a particular material. Detection of orbital angular momentums provide an indication of the associated material concentration that is being monitored by the apparatus. Each of the rings 1020 represents a different concentration of a selected material that is being monitored. Each of the Eigen modes has a Poynting vector 1022 for generating the rings indicating different material concentrations.

Referring now to FIG. 11, there is illustrated a block diagram of the apparatus for providing concentration measurements of various materials responsive to the orbital angular momentum detected by the apparatus in accordance with the principles described herein above. An emitter 1102 transmits wave energy 1104 that comprises a series of plane waves. The emitter 1102 may provide a series of plane waves such as those describes previously with respect to FIG. 3. The orbital angular momentum generation circuitry 1106 generates a series of waves having an orbital angular momentum applied to the waves 1108 in a known manner. The orbital angular momentum generation circuitry 706 may utilize holograms or some other type of orbital angular momentum generation process as will be more fully described herein below. The orbital angular momentum twisted waves 708 are applied to a sample material 1110 under test. The sample material 1110 contains a material, and the concentration of the material is determined via a concentration detection apparatus in accordance with the process described herein.

A series of output waves 1112 from the sample material 710 exit the sample and have a particular orbital angular momentum imparted thereto as a result of the concentration of the particular material under study within the sample material 710. The output waves 1112 are applied to a matching module 1114 that includes a mapping aperture for amplifying a particular orbital angular momentum generated by the specific material under study. The matching module 1114 will amplify the orbital angular momentums associated with the particular concentration of material that is detected by the apparatus. The amplified OAM waves 1116 are provided to a detector 1118. The detector 1118 detects OAM waves relating to the concentration of a material within the sample and provides this concentration information to a user interface 1120. The user interface 1120 interprets the concentration information and provides relevant concentration indication to an individual or a recording device.

Referring now to FIG. 12, there is more particularly illustrated the emitter 1102. The emitter 1102 may emit a number of types of energy waves 1104 to the OAM generation module 1106. The emitter 1102 may emit optical waves 1200, electromagnetic waves 1202, acoustic waves 1204 or any other type of particle waves 1206. The emitted waves 1104 are plane waves such as those illustrated in FIG. 7 having no orbital angular momentum applied thereto and may come from a variety of types of emission devices and have information included therein. In one embodiment, the emission device may comprise a laser. Plane waves have wavefronts that are parallel to each other having no twist or helicity applied thereto, and the orbital angular momentum of the wave is equal to 0. The Poynting vector within a plane wave is completely in line with the direction of propagation of the wave.

The OAM generation module 1106 processes the incoming plane wave 1104 and imparts a known orbital angular momentum onto the plane waves 1104 provided from the emitter 1102. The OAM generation module 1106 generates twisted or helical electromagnetic, optic, acoustic or other types of particle waves from the plane waves of the emitter 702. A helical wave 1108 is not aligned with the direction of propagation of the wave but has a procession around direction of propagation as shown in FIG. 5. The OAM generation module 1106 may comprise in one embodiment a fixed orbital angular momentum generator 1302 as illustrated in FIG. 13. The fixed orbital angular momentum generator 1302 receives the plane waves 1104 from the emitter 1102 and generates an output wave 1304 having a fixed orbital angular momentum applied thereto.

The fixed orbital angular momentum generator 1302 may in one embodiment comprise a holographic image for applying the fixed orbital angular momentum to the plane wave 1104 in order to generate the OAM twisted wave 904. Various types of holographic images may be generated in order to create the desired orbital angular momentum twist to an optical signal that is being applied to the orbital angular momentum generator 1102. Various examples of these holographic images are illustrated in FIG. 14a-14d . In one embodiment, the conversion of the plane wave signals transmitted from the emitter 1102 by the orbital angular momentum generation circuitry 706 may be achieved using holographic images.

Most commercial lasers emit an HG₀₀ (Hermite-Gaussian) mode 1502 (FIG. 15) with a planar wave front and a transverse intensity described by a Gaussian function. Although a number of different methods have been used to successfully transform an HG₀₀ Hermite-Gaussian mode 1502 into a Laguerre-Gaussian mode 1504, the simplest to understand is the use of a hologram.

The cylindrical symmetric solution u_(pl) (r,φ,z) which describes Laguerre-Gaussian beams, is given by the equation:

${{u_{pl}\left( {r,\varphi,z} \right)}\quad} = {\quad{\quad{\quad{{\frac{C}{\left( {1 + {z^{2}\text{/}z_{R}^{2}}} \right)^{1/2}}\left\lbrack \frac{r\sqrt{2}}{w(z)} \right\rbrack}^{l}{L_{p}^{l}\left\lbrack \frac{2r^{2}}{w^{2}(z)} \right\rbrack}{\exp\left\lbrack \frac{- r^{2}}{w^{2}(z)} \right\rbrack} {\exp\left\lbrack \frac{{- {ikr}^{2}}z}{2\left( {z^{2} + z_{R}^{2}} \right)} \right\rbrack}{\exp \left( {{- {il}}\; \varphi} \right)} \times {\exp\left\lbrack {{i\left( {{2p} + l + 1} \right)}\tan^{- 1}\frac{z}{z_{R}}} \right\rbrack}}}}}$

Where z_(R) is the Rayleigh range, w(z) is the radius of the beam, L_(P) is the Laguerre polynomial, C is a constant, and the beam waist is at z=0.

In its simplest form, a computer generated hologram is produced from the calculated interference pattern that results when the desired beam intersects the beam of a conventional laser at a small angle. The calculated pattern is transferred to a high resolution holographic film. When the developed hologram is placed in the original laser beam, a diffraction pattern results. The first order of which has a desired amplitude and phase distribution. This is one manner for implementing the OAM generation module 1106. A number of examples of holographic images for use within a OAM generation module are illustrated with respect to FIGS. 14a -14 e.

There are various levels of sophistication in hologram design. Holograms that comprise only black and white areas with no grayscale are referred to as binary holograms. Within binary holograms, the relative intensities of the two interfering beams play no role and the transmission of the hologram is set to be zero for a calculated phase difference between zero and π, or unity for a phase difference between π and 2π. A limitation of binary holograms is that very little of the incident power ends up in the first order diffracted spot, although this can be partly overcome by blazing the grating. When mode purity is of particular importance, it is also possible to create more sophisticated holograms where the contrast of the pattern is varied as a function of radius such that the diffracted beam has the required radial profile.

A plane wave shining through the holographic images 1402 will have a predetermined orbital angular momentum shift applied thereto after passing through the holographic image 1402. OAM generator 1102 is fixed in the sense that a same image is used and applied to the beam being passed through the holographic image. Since the holographic image 1402 does not change, the same orbital angular momentum is always applied to the beam being passed through the holographic image 1402. While FIG. 14a-14e illustrate a number of embodiments of various holographic images that might be utilized within the orbital angular momentum generator 1102, it will be realized that any type of holographic image 1402 may be utilized in order to achieve the desired orbital angular momentum within an beam being shined through the image 1402.

In another example of a holographic image illustrated in FIG. 16, there is illustrated a hologram that utilizes two separate holograms that are gridded together to produce a rich number of orbital angular momentum (l). The superimposed holograms of FIG. 16 have an orbital angular momentum of l=1 and l=3 which are superimposed upon each other to compose the composite vortex grid 1602. The holograms utilized may also be built in a manner that the two holograms are gridded together to produce a varied number of orbital angular momentums (l) not just on a line (l=+1, l=0, l=−1) but on a square which is able to identify the many variables more easily. Thus, in the example in FIG. 16, the orbital angular momentums along the top edge vary from +4 to +1 to −2 and on the bottom edge from +2 to −1 to −4. Similarly, along the left edge the orbital angular momentums vary from +4 to +3 to +2 and on the right edge from −2 to −3 to −4. Across the horizontal center of the hologram the orbital angular momentums provided vary from +3 to 0 to −3 and along the vertical axis vary from +1 to 0 to −1. Thus, depending upon the portion of the grid a beam may pass through, varying orbital angular momentum may be achieved.

Referring now to FIG. 17, in addition to a fixed orbital angular momentum generator, the orbital angular momentum generation circuitry 1106 may also comprise a tunable orbital angular momentum generator circuitry 1702. The tunable orbital angular momentum generator 1702 receives the input plane wave 1104 but additionally receives one or more tuning parameters 1704. The tuning parameters 1704 tune the tunable OAM generator 1702 to apply a selected orbital angular momentum so that the tuned OAM wave 1706 that is output from the OAM generator 1702 has a selected orbital angular momentum value applied thereto.

This may be achieved in any number of fashions. In one embodiment, illustrated in FIG. 18, the tunable orbital angular momentum generator 1002 may include multiple hologram images 1802 within the tunable OAM generator 1702. The tuning parameters 1704 enable selection of one of the holographic images 1806 in order to provide the desired OAM wave twisted output signal 1706 through a selector circuit 1804. Alternatively, the gridded holographic image such as that described in FIG. 16 may be utilized and the beam shined on a portion of the gridded image to provide the desired OAM output. The tunable OAM generator 1702 has the advantage of being controlled to apply a particular orbital angular momentum to the output orbital angular momentum wave 1706 depending upon the provided input parameter 1704. This enables the concentrations of a variety of different materials to be monitored, or alternatively, for various different concentrations of the same material to be monitored.

Referring now to FIG. 18, there is more particularly implemented a block diagram of a tunable orbital angular momentum generator 1702. The generator 1702 includes a plurality of holographic images 1802 for providing orbital angular momentums of various types to a provided light signal. These holographic images 1802 are selected responsive to a selector circuitry 1804 that is responsive to the input tuning parameters 1704. The selected filter 1806 comprises the holographic image that has been selected responsive to the selector controller 1804 and receives the input plane waves 1104 to provide the tuned orbital angular momentum wave output 1706. In this manner, signals having a desired orbital angular momentum may be output from the OAM generation circuitry 1106.

Referring now to FIG. 19, there is illustrated the manner in which the output of the OAM generator 1106 may vary a signal by applying different orbital angular momentum thereto. FIG. 19 illustrates helical phase fronts in which the Poynting vector is no longer parallel to the beam axis and thus has an orbital angular momentum applied thereto. In any fixed radius within the beam, the Poynting vector follows a spiral trajectory around the axis. Rows are labeled by 1, the orbital angular momentum quantum number, L=l

is the beams orbital angular momentum per photon within the output signal. For each l, the left column 1902 is the light beam's instantaneous phase. The center column 1904 comprises the angular intensity profiles and the right column 1906 illustrates what occurs when such a beam interferes with a plane wave and produces a spiral intensity pattern. This is illustrated for orbital angular momentums of −1, 0, 1, 2 and 3 within the various rows of FIG. 19.

Referring now to FIG. 20, there is illustrated an alternative manner in which the OAM generator 1106 may convert a Hermite-Gaussian beam output from an emitter 1102 to a Laguerre-Gaussian beams having imparted therein an orbital angular momentum using mode converters 2004 and a Dove prism 2010. The Hermite-Gaussian mode plane waves 2002 are provided to a π/2 mode convertor 2004. The π/2 mode convertor 2004 produce beams in the Laguerre-Gaussian modes 2006. The Laguerre-Gaussian modes beams 2006 are applied to either a it mode convertor 2008 or a dove prism 2010 that reverses the mode to create a reverse Laguerre-Gaussian mode signal 2012.

Referring now to FIG. 21, there is illustrated the manner in which holograms within the OAM generator 1106 generate a twisted light beam. A hologram 2102 can produce light beam 2104 and light beam 2106 having helical wave fronts and associated orbital angular momentum l

per photon. The appropriate hologram 2102 can be calculated or generated from the interference pattern between the desired beam form 2104, 2106 and a plane wave 2108. The resulting holographic pattern within the hologram 2102 resembles a diffraction grating, but has a l-pronged dislocation at the beam axis. When the hologram is illuminated with the plane wave 2108, the first-order diffracted beams 2104 and 2106 have the desired helical wave fronts to provide the desired first ordered diffracted beam display 2110.

Referring now to FIG. 22, there is more particularly illustrated the manner in which the sample 1110 receives the input OAM twisted wave 1108 provided from the OAM generator 1106 and provides an output OAM wave 1112 having a particular OAM signature associated therewith that depends upon the concentration of a particular monitored material within the sample 1110. The sample 1110 may comprise any sample that is under study and may be in a solid form, liquid form or gas form. The sample material 1110 that may be detected using the system described herein may comprise a variety of different materials. As stated previously, the material may comprise liquids such as blood, water, oil or chemicals. The various types of carbon bondings such as C—H, C—O, C—P, C—S or C—N may be provided for detection. The system may also detect various types of bondings between carbon atoms such as a single bond (methane or Isooctane), dual bond items (butadiene and benzene) or triple bond carbon items such as acetylene.

The sample 1110 may include detectable items such as organic compounds including carbohydrates, lipids (cylcerol and fatty acids), nucleic acids (C,H,O,N,P) (RNA and DNA) or various types of proteins such as polyour of amino NH₂ and carboxyl COOH or aminos such as tryptophan, tyrosine and phenylalanine. Various chains within the samples 1110 may also be detected such as monomers, isomers and polymers. Enzymes such as ATP and ADP within the samples may be detected. Substances produced or released by glands of the body may be in the sample and detected. These include items released by the exocrine glands via tube/ducts, endocrine glands released directly into blood samples or hormones. Various types of glands that may have their secretions detected within a sample 1110 include the hypothalamus, pineal and pituitary glands, the parathyroid and thyroid and thymus, the adrenal and pancreas glands of the torso and the hormones released by the ovaries or testes of a male or female.

The sample 1110 may also be used for detecting various types of biochemical markers within the blood and urine of an individual such as melanocytes and keratinocytes. The sample 1110 may include various parts of the body to detect defense substances therein. For example, with respect to the skin, the sample 1110 may be used to detect carotenoids, vitamins, enzymes, b-carotene and lycopene. With respect to the eye pigment, the melanin/eumelanin, dihydroxyindole or carboxylic may be detected. The system may also detect various types of materials within the body's biosynthetic pathways within the sample 1110 including hemoglobin, myoglobin, cytochromes, and porphyrin molecules such as protoporphyrin, coporphyrin, uroporphyrin and nematoporphyrin. The sample 1110 may also contain various bacterial to be detected such as propion bacterium, acnes. Also various types of dental plaque bacteria may be detected such as porphyromonos gingivitis, prevotella intremedi and prevotella nigrescens. The sample 1110 may also be used for the detection of glucose in insulin within a blood sample 1110.

The orbital angular momentum within the beams provided within the sample 1110 may be transferred from light to matter molecules depending upon the rotation of the matter molecules. When a circularly polarized laser beam with a helical wave front traps a molecule in an angular ring of light around the beam axis, one can observe the transfer of both orbital and spin angular momentum. The trapping is a form of optical tweezing accomplished without mechanical constraints by the ring's intensity gradient. The orbital angular momentum transferred to the molecule makes it orbit around the beam axis as illustrated at 2302 of FIG. 23. The spin angular momentum sets the molecule spinning on its own axis as illustrated at 2304.

The output OAM wave 1112 from the sample 1110 will have an orbital angular momentum associated therewith that is different from the orbital angular momentum provided on the input OAM wave 1108. The difference in the output OAM wave 1112 will depend upon the material contained within the sample 1110 and the concentration of these materials within the sample 1110. Differing materials of differing concentration will have unique orbital angular momentums associated therewith. Thus, by analyzing the particular orbital angular momentum signature associated with the output OAM wave 1112, determinations may be made as to the materials present within the sample 1110 and the concentration of these materials within the sample may also be determined.

Referring now to FIG. 24, the matching module 1114 receives the output orbital angular momentum wave 1112 from the sample 1110 that has a particular signature associated therewith based upon the orbital angular momentum imparted to the waves passing through the sample 1110. The matching module 1114 amplifies the particular orbital angular momentum of interest in order to provide an amplified wave having the desired orbital angular momentum of interest 2416 amplified. The matching module 1114 may comprise a matching aperture that amplifies the detection orbital angular momentum associated with a specific material or characteristic that is under study. The matching module 1114 may in one embodiment comprise a holographic filter such as that described with respect to FIGS. 14a-14d in order to amplify the desired orbital angular momentum wave of interest. The matching module 1114 is established based upon a specific material of interest that is trying to be detected by the system. The matching module 1114 may comprise a fixed module using holograms as illustrated in FIGS. 14a-14d or a tunable module in a manner similar to that discussed with respect to the OAM generation module 1106. In this case, a number of different orbital angular momentums could be amplified by the matching module in order to detect differing materials or differing concentration of materials within the sample 1110. Other examples of components for the matching module 1114 include the use of quantum dots, nanomaterials or metamaterials in order to amplify any desired orbital angular momentum values within a received wave form from the sample 1110.

Referring now to FIG. 25, the matching module 1114 rather than using holographic images in order to amplify the desired orbital angular momentum signals may use non-linear crystals in order to generate higher orbital angular momentum light beams. Using a non-linear crystal 2502, a first harmonic orbital angular momentum beam 2504 may be applied to a non-linear crystal 2502. The non-linear crystal 2502 will create a second order harmonic signal 2506.

Referring now to FIG. 26, there is more particularly illustrated the detector 1118 to which the amplified orbital angular momentum wave 1116 from the matching circuit 1114 in order that the detector 1118 may extract desired OAM measurements 2602. The detector 1118 receives the amplified OAM waves 1116 and detects and measures observable changes within the orbital angular momentum of the emitted waves due to the concentration of a particular material under study within the sample 1110. The detector 1118 is able to measure observable changes within the emitted amplified OAM wave 1116 from the state of the input OAM wave 1108 applied to the sample 1110. The extracted OAM measurements 2602 are applied to the user interface 1120. The manner in which the detector 1118 may detect differences within the orbital angular momentum is more particularly illustrates with respect to FIG. 27-29.

FIG. 27 illustrates the difference in impact between spin angular polarization and orbital angular polarization due to passing of a beam of light through a sample 2702. In sample 2702 a, there is illustrated the manner in which spin angular polarization is altered responsive to a beam passing through the sample 2702 a. The polarization of a wave having a particular spin angular momentum 2704 passing through the sample 2702 a will rotate from a position 2704 to a new position 2706. The rotation occurs within the same plane of polarization. In a similar manner, as illustrated with respect to sample 2702 b, an image appears as illustrated generally at 2708 before it passes through the sample 2702 b. Upon passing the image through the sample 2702 b the image will rotate from the position illustrated at 2710 to a rotated position illustrated at 2712. The amount of rotation is dependent upon the level of concentration of the material being detected within the sample 2702. Thus, as can be seen with respect to the sample 2702 of FIG. 27, both the spin angular polarization and the orbital angular momentum will change based upon the concentration of materials within the sample 2702. By measuring the amount of rotation of the image caused by the change in orbital angular momentum, the concentration of a particular material may be determined.

This overall process can be more particularly illustrated in FIG. 28. A light source 2802 shines a light beam through expanding optics 2804. The expanded light beam is applied through a metalab generated hologram 2806 that imparts an orbital angular momentum to the beam. The twisted beam from the hologram 2806 is shined through a sample 2808 having a particular length L. This causes the generation of a twisted beam on the output side of the sample 2808 to create a number of detectable waves having various orbital angular momentums 2810 associated therewith. The image 2812 associated with the light beam that is applied to sample 2808 will rotate an angle φ depending upon the concentration of the material within the sample 2808. The rotation φ of the image 2812 is different for each value orbital angular momentum −l or +l. The change in rotation of the image Δφ may be described according to the equation:

Δφ=φ₁−φ⁻¹ =f(l,L,C)

Where l is orbital angular momentum number, L is the path length of the sample and C is the concentration of the material being detected.

Thus, since the length of the sample L is known and the orbital angular momentum may be determined using the process described herein, these two pieces of information may be able to calculate a concentration of the material within the provided sample.

The above equation may be utilized within the user interface more particularly illustrated in FIG. 29. The user interface 1120 processes the OAM measurements 2502 using an internal algorithm 2902 that provides for the generation of concentration information 2904 that may be displayed in some type of user display. The algorithm would in one embodiment utilize that equation described herein above in order to determine the concentration based upon the length of a sample and the detected variation in orbital angular momentum. The process for calculating the concentration may be done in a laboratory setting where the information is transmitted wirelessly to the lab or the user interface can be associated with a wearable device connected to a meter or cell phone running an application on the cell phone connected via a local area network or wide area network to a personal or public cloud. The user interface 2920 of the device can either have a wired or wireless connection utilizing Bluetooth, ZigBee or other wireless protocols.

Referring now to FIG. 30, there is illustrated the manner in which the various data accumulated within the user interface 1120 that has been collected in the manner described herein above may be stored and utilized for higher level analysis. Various devices 3002 for collecting data as described herein above may communicate via private network clouds 3004 or with a public cloud 3006. When communicating with a private cloud 3004, the devices 3002 merely store information that is associated with a particular user device that is for use with respect to analysis of the user associated with that user device. Thus, an individual user could be monitoring and storing information with respect to their present glucose concentrations in order to monitor and maintain their diabetes.

Alternatively, when information is compiled from multiple devices 3002 within the public cloud 3006, this information may be provided directly to the public cloud 3006 from the individual devices 3002 or through the private clouds 3004 of the associated network devices 3002. Utilizing this information within the public cloud 3006 large databases may be established within servers 3008 associated with the public cloud 3006 to enable large scale analysis of various health related issues associated with the information processed from each of the individual devices 3002. This information may be used for analyzing public health issues.

Thus, the user interface 1120 in addition to including the algorithm 2902 for determining concentration information 2904 will include a wireless interface 2906 enabling the collected information to be wirelessly transmitted over the public or private cloud as described with respect to FIG. 30. Alternatively, the user interface may comprise a storage database 2908 enabling the collected information to be locally stored rather than transmitted wirelessly to a remote location.

Referring now to FIG. 31, there is illustrated a particular example of a block diagram of a particular apparatus for measuring the concentration of glucose using the orbital angular momentum of photons of a light beam shined through a glucose sample. The process creates a second-order harmonic with helical light beam using a non-linear crystal such as that described with respect to FIG. 25. The emission module 2402 generates plain electromagnetic waves that are provided to an OAM generation module 3104. The OAM generation module 3104 generates light waves having an orbital angular momentum applied thereto using holograms to create a wave having an electromagnetic vortex. The OAM twisted waves are applied to the sample 3106 that is under study in order to detect the glucose concentration within a sample of blood. A rotated signature exits the sample 3106 in the manner described previously with respect to FIGS. 27-28 and is provided to the matching module 3108. The matching module 3108 will amplify the orbital angular momentum such that the observed concentrations may be calculated from the orbital momentum of the signature of the glucose. These amplified signals are provided to detection module 3110 which measures the radius of the beam w(z) or the rotation of the image provided to the sample via the light beam. This detected information is provided to the user interface that include a sensor interface wired or wireless Bluetooth or ZigBee connection to enable the provision of the material to a reading meter or a user phone for the display of concentration information with respect to the sample.

In this manner concentrations of various types of material as describe herein may be determined utilizing the orbital angular momentum signatures of the samples under study and the detection of these materials or their concentrations within the sample determine as described.

It will be appreciated by those skilled in the art having the benefit of this disclosure that this system and method for making concentration measurements within a sample material using orbital angular momentum provides a non-invasive manner for detecting material concentration. It should be understood that the drawings and detailed description herein are to be regarded in an illustrative rather than a restrictive manner, and are not intended to be limiting to the particular forms and examples disclosed. On the contrary, included are any further modifications, changes, rearrangements, substitutions, alternatives, design choices, and embodiments apparent to those of ordinary skill in the art, without departing from the spirit and scope hereof, as defined by the following claims. Thus, it is intended that the following claims be interpreted to embrace all such further modifications, changes, rearrangements, substitutions, alternatives, design choices, and embodiments. 

What is claimed is:
 1. An apparatus for identifying a concentration of a specific material within a first material, comprising: an input for receiving a signal after the signal passes through the first material, the signal having at least one orthogonal function therein, the at least one orthogonal function comprised of at least one of an orbital angular momentum function or a Laguerre-Gaussian function; a detector for detecting the at least one orthogonal function within the signal, for determining the concentration of the specific material within the first material based upon the detected at least one orthogonal function and for generating an indication responsive to the determination; and an output for providing the generated indication.
 2. The detector of claim 1 further including an amplifier that receives the first signal that has passed through the first material and amplifies a first portion of the first signal having the at least one orthogonal function associated therewith.
 3. The detector of claim 2, wherein the amplifier further includes a hologram that amplifies the first portion of the first signal.
 4. The detector of claim 1, wherein the detector further comprises: an orthogonal function detector that determines the detected orthogonal function within the first signal from the first material; and a processor that determines the concentration of the material within the first material responsive to the detected orthogonal function.
 5. The detector of claim 4, further including a user interface associated with the processor comprising: a set of computer instructions that configures the processor to determine the concentration of the material within the first material responsive to the detected orthogonal function; and a database that stores concentration data from the concentration of the material determined by the processor.
 6. The detector of claim 1, wherein the first signal comprises a light beam.
 7. The detector of claim 1, wherein the detector further identifies the material within the first material responsive to the detected at least one orthogonal function and generates the indication responsive to the identification.
 8. The detector of claim 1, wherein the detector detects the at least one orthogonal function by interfering plane waves with helical waves within the signal.
 9. The detector of claim 1, wherein the detector determines the concentration of the specific material by determining a signature of the at least one orthogonal function and determining the concentration based upon the determined signature of the detected at least one orthogonal function.
 10. The detector of claim 1, wherein a frequency of the received signal magnifies a signature of the detected at least one orthogonal function.
 11. A method for identifying a specific material, comprising receiving a signal after the signal passes through the first material, the signal having at least one orthogonal function therein, the at least one orthogonal function comprised of at least one of an orbital angular momentum function or a Laguerre-Gaussian function; detecting the at least one orthogonal function within the signal; determining the concentration of the specific material within the first material based upon the detected at least one orthogonal function; generating an indication responsive to the determination; and providing the generated indication.
 12. The method of claim 11 further including amplifying a first portion of the first signal having the at least one orthogonal function associated therewith.
 13. The method of claim 12, wherein the step of amplifying further comprises amplifying the first portion of the first signal using a hologram.
 14. The method of claim 13 further including storing concentration data from the determined concentration of the material.
 15. The method of claim 11, wherein the first signal comprises a light beam.
 16. The method of claim 11, wherein the step of determining further comprises identifying the material within the first material responsive to the detected at least one orthogonal function.
 17. The method of claim 16, wherein the step of providing further comprises generating the indication responsive to the identification.
 18. The method of claim 11, wherein the step of detecting further comprises interfering plane waves with helical waves within the signal to detect the at least one orthogonal function.
 19. The method of claim 11, wherein the step of determining further comprises determining a signature of the at least one orthogonal function and determining the concentration based upon the determined signature of the detected at least one orthogonal function.
 20. The method of claim 11, further comprising magnifying a signature of the detected at least one orthogonal function using a frequency of the received signal.
 21. An apparatus for identifying a specific material within a first material, comprising: an input for receiving a signal after the signal passes through the first material, the signal having at least one orthogonal function therein, the at least one orthogonal function comprised of at least one of an orbital angular momentum function or a Laguerre-Gaussian function; a detector for detecting the at least one orthogonal function within the signal, for identifying the specific material within the first material based upon the detected at least one orthogonal function and for generating an indication responsive to the identification; and an output for providing the generated indication. 